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String Theory Demystified

String Theory Demystified

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CHAPTER 4<br />

<strong>String</strong> Quantization<br />

At this point we have the classical physics of the string in place. The next step<br />

toward a quantum theory is, of course, to quantize the string. We will start off by<br />

looking at a quantum theory of a single string. From quantum fi eld theory you recall<br />

that this procedure is known as fi rst quantization. This is opposed to the procedure<br />

called second quantization, which is a viewpoint of quantizing fi elds (see Quantum<br />

Field <strong>Theory</strong> Demystifi ed for a review). The difference in the two approaches will<br />

be on how we view the X m (s, t ). If we take them to be fi elds, then the quantization<br />

procedure is second quantization. If we take them to be space-time coordinates, as<br />

we have so far, then the process is fi rst quantization. This is the procedure we will<br />

apply in this chapter. There are several different approaches to quantization of the<br />

string, each with their own accompanying diffi culties and problems. The main<br />

approaches used are called covariant quantization, light-cone quantization, and<br />

BRST quantization. We consider the fi rst two approaches here, and will discuss<br />

BRST quantization later.<br />

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